Optical analog-to-digital converter, method of constructing the same, optical signal demodulator, and optical modulator-demodulator

ABSTRACT

An optical A/D converter according to the present invention includes an optical splitter that splits an analog input signal light into plurals, a plurality of Mach-Zehnder interferometers to which each of the signal lights split by the optical splitter is input, and plurality of optical/electrical conversion unit that convert each signal lights output from each Mach-Zehnder interferometer into a digital electrical signal, in which each Mach-Zehnder interferometer includes optical intensity-to-phase conversion unit that optically convert intensity of the input signal light into an amount of phase shift and the amount of phase shift differs for each Mach-Zehnder interferometer. Then, it is possible to provide a high speed and low power consuming optical demodulation circuit.

TECHNICAL FIELD

The present invention relates to an optical analog-to-digital converter, an optical signal demodulator and an optical modulator-demodulator using thereof, and a method of constructing the optical analog-to-digital converter that are used in an optical communication system and optical interconnection.

BACKGROUND ART

Improvement in the speed and increase in the capacity by wavelength division multiplexing is further progressing in the optical communication system in intermediate and long distances. The current main optical communication system uses wavelength division multiplex communication with determined wavelength channel spacing. Therefore, with 50 GHz spacing in the band of an optical fiber amplifier, approximately 100 channels can be used.

When the channel spacing is Δf[Hz] and the transmission rate is B[bit/s], B/Δf[bit/s/Hz] shall be spectral efficiency. When Δf=50 GHz and the transmission rate is 100 Gbit/s for each channel, the spectral efficiency will be 2 bit/s/Hz.

As the band of the optical fiber amplifier is limited, it is necessary to improve the spectral efficiency. However, simply increasing the bit rate of a signal in order to improve the spectral efficiency raises a problem of interchannel crosstalk. Thus, study on optical multi-level modulation and optical OFDM (Orthogonal Frequency-Division Multiplexing) has been progressing as a next generation optical communication system. The optical multi-level modulation is a method to increase the amount of information by multi-leveling using an amplitude and a phase of a light without increasing the spectral band unlike optical intensity modulation of a related art using two values of 0 and 1. Moreover, in the optical OFDM, an OFDM signal is generated by an electrical signal and is optically modulated, and optical subcarriers are set in an orthogonal state to multiplex. This solves the crosstalk problem, thereby improves the spectral efficiency.

An optical signal with multi-leveling and multiplexing mainly involving electrical signal processing in this way is transmitted and demodulated into an electrical signal by a receiver. An analog-to-digital (A/D) converter is required in the subsequent stage of a PD (photodiode) of an optical demodulation circuit. Currently, an A/D converter using an electrical circuit is commonly used.

On the other hand, there are many proposals for the optical A/D converter that directly derives analog quantity of an optical signal as a digital value because of the feature of rapidity included therein. For example, Patent Literature 1 splits an optical signal by different predetermined split ratios to represent the amount of a light by a predetermined ratio and detects an optical analog quantity of the input optical signal by evaluating whether each split optical signal reaches a threshold.

Further, Patent literature 2 composes in optical A/D conversion means a feedback system through a nonlinear optical element for an input optical signal, which is an analog signal, and thus a first output light, which is a digital signal, is sequentially obtained from the optical A/D conversion means.

In Patent Literature 3, an optical coding circuit optically codes pulse trains of a signal light having a first wavelength according to control light, which is pulse trains of a light analog signal having a nearby second wavelength different from the first wavelength and is optically sampled, by a plurality of optical coders provided with optical nonlinear elements having periodic characteristics whose input and output characteristics regarding optical intensity are different, and outputs the pulse trains of the plurality of optically coded signal lights from each optical coder. Then, an optical quantization circuit outputs pulse trains of a carrier light having a nearby third wavelength that is different from the first wavelength as an optical digital signal after conducting optical threshold processing according to the pulse trains of the plurality of optically coded signal lights and optical quantization using a plurality of optical threshold processing devices provided with optical nonlinear elements which are respectively connected to each optical coder and have periodic input and output characteristics regarding the optical intensity.

Patent Literature 4 is characterized in that a plurality of interference optical modulators are included, a photovoltaic element is formed on the same substrate, and an output voltage of this photovoltaic element is applied on the interference optical modulators. Therefore, in this example, a PD receives an intensity signal light once and converts the intensity signal light into a voltage signal, thereby determining the speed of the entire circuit by the speed of this electrical signal.

Patent Literature 5 discloses a technique to sample a signal light using probe light and perform A/D conversion. Moreover, Patent Literature 6 discloses a technique to successively perform A/D conversion by light subtraction.

CITATION LIST Patent Literature

-   Patent Literature 1: Japanese Unexamined Patent Application     Publication No. 2007-24924 -   Patent Literature 2: Japanese Unexamined Patent Application     Publication No. 1-56426 -   Patent Literature 3: Japanese Unexamined Patent Application     Publication No. 2005-173530 -   Patent Literature 4: Japanese Utility Model No. 61-203566 -   Patent Literature 5: Japanese Unexamined Patent Application     Publication No. 2008-209775 -   Patent Literature 6: Japanese Unexamined Patent Application     Publication No. 2001-051314

SUMMARY OF INVENTION Technical Problem

When the A/D converter disposed in the subsequent stage of the PD in an optical demodulation circuit on the receiver side uses an electrical circuit, multi-leveled and multiplexed transmissions mainly involving electrical signal processing with an increased optical transmission capacity is limited to the speed of the electrical signal processing. For example, in a reported instance of an electrical OFDM, the bit rate of each subcarrier remains below Gbit/s. Additionally, there has been a problem that the power consumption for processing is large.

On the other hand, the method of using the optical A/D converter is considered to have a complicated configuration due to the difficulty of subtracting a light with given intensity from a light with some intensity.

The present invention is made in view of the above circumstances and its object is to provide an optical demodulation circuit using a high speed and low power consuming optical A/D converter.

Solution to Problem

An optical A/D converter according to the present invention includes:

an optical splitter that splits an input analog optical signal into plurals,

a plurality of Mach-Zehnder interferometers to which each of the optical signals split by the optical splitter is input,

plurality of optical/electrical conversion unit that convert each optical signal output from each Mach-Zehnder interferometer into a digital electrical signal, in which

each Mach-Zehnder interferometer comprises optical intensity-to-phase conversion unit that optically converts intensity of the input optical signal into an amount of phase shift, and

the amount of phase shift differs for each Mach-Zehnder interferometer.

A method of constructing an optical A/D converter according to the present invention comprises:

providing an optical splitter that splits an input analog optical signal into plurals,

providing a plurality of Mach-Zehnder interferometers, each of the optical signals split by the optical splitter being input to the plurality of Mach-Zehnder interferometers,

providing plurality of optical/electrical conversion unit that convert each optical signal output from each Mach-Zehnder interferometer into a digital electrical signal,

providing optical intensity-to-phase conversion unit to each Mach-Zehnder interferometer, in which the optical intensity-to-phase conversion unit optically converts intensity of the input optical signal into an amount of phase shift, and

performing construction so that the amount of phase shift will be different for each Mach-Zehnder interferometer.

Advantageous Effects of Invention

According to the present invention, it is possible to obtain a high-speed and low power consuming optical A/D converter and realizes an optical signal demodulator and an optical modulator-demodulator with the optical A/D converter included therein at a high speed with low power.

BRIEF DESCRIPTION OF DRAWINGS

FIG. 1 is a block diagram of an optical A/D converter according to a first exemplary embodiment;

FIG. 2A is a diagram showing a configuration of an optical modulation region 5 in FIG. 1;

FIG. 2B is a diagram showing a configuration of an optical modulation region 6 in FIG. 1;

FIG. 2C is a diagram showing a configuration of an optical modulation region 7 in FIG. 1;

FIG. 2D is a diagram showing a configuration of an optical modulation region 8 in FIG. 1;

FIG. 3 is a graph showing features included in optical intensity-to-phase conversion units 25 to 28;

FIG. 4 is a graph showing relative optical intensity on a cross-section 21 in FIG. 1;

FIG. 5 is a diagram showing digital signals depending on input optical intensity output from an optical A/D converter according to first, second, and third exemplary embodiments;

FIG. 6 is a block diagram of the optical A/D converter according to the second exemplary embodiment;

FIG. 7A is a diagram showing a configuration of an optical modulation region 35 in FIG. 6;

FIG. 7B is a diagram showing a configuration of an optical modulation region 36 in FIG. 6;

FIG. 7C is a diagram showing a configuration of an optical modulation region 37 in FIG. 6;

FIG. 7D is a diagram showing a configuration of an optical modulation region 38 in FIG. 6;

FIG. 7E is a diagram showing a configuration of an optical intensity-to-phase converter 39;

FIG. 7F is a diagram showing another configuration of the optical intensity-to-phase converter 39;

FIG. 8 is a block diagram of the optical A/D converter according to the third exemplary embodiment;

FIG. 9A is a diagram showing a configuration of an optical modulation region 55 in FIG. 8;

FIG. 9B is a diagram showing a configuration of an optical modulation region 56 in FIG. 8;

FIG. 9C is a diagram showing a configuration of an optical modulation region 57 in FIG. 8;

FIG. 9D is a diagram showing a configuration of an optical modulation region 58 in FIG. 8;

FIG. 9E is a diagram showing a configuration of an optical intensity-to-phase converter 59;

FIG. 10A is a diagram showing a configuration of the optical modulation region 5 in FIG. 1 corresponding to a digital code in FIG. 12;

FIG. 10B is a diagram showing a configuration of the optical modulation region 6 in FIG. 1 corresponding to a digital code in FIG. 12;

FIG. 10C is a diagram showing a configuration of the optical modulation region 7 in FIG. 1 corresponding to a digital code in FIG. 12;

FIG. 10D is a diagram showing a configuration of the optical modulation region 8 in FIG. 1 corresponding to a digital code in FIG. 12;

FIG. 11A is a diagram showing a configuration of the optical modulation region 35 in FIG. 6 corresponding to a digital code in FIG. 12;

FIG. 11B is a diagram showing a configuration of the optical modulation region 36 in FIG. 6 corresponding to a digital code in FIG. 12;

FIG. 11C is a diagram showing a configuration of the optical modulation region 37 in FIG. 6 corresponding to a digital code in FIG. 12;

FIG. 11D is a diagram showing a configuration of the optical modulation region 38 in FIG. 6 corresponding to a digital code in FIG. 12; and

FIG. 12 is a diagram showing digital signals different from FIG. 5 that can be output in the first, second, and third exemplary embodiments.

DESCRIPTION OF EMBODIMENTS

It is necessary to detect the state of a phase and an amplitude of a light in order to demodulate a multi-leveled and multiplexed optical signal. However, as it is difficult to detect the state of a light on a complex plane, generally a preceding stage separates the optical signal into a real part I and an imaginary part Q and a receiver (PD) detects intensity information of the respective real part I and imaginary part Q.

For example, the technique of coherent optical detection uses a device called an optical phase hybrid that makes four beams of local lights having phases different by 90 degrees respectively interfere with a signal light, obtains two beams each of output lights for the real part I and the imaginary part Q, and a PD (Photodiode) receives the two beams each of lights. The present invention performs optical A/D conversion using intensity information in the two each of the lights after the optical signal is already separated into the real part I or the imaginary part Q.

Detection of optical intensity has previously been carried out by a PD receiving and converting a light into an electrical signal, and the electrical signal is converted into a digital value by an A/D converter by an electrical circuit. The method of using the optical A/D converter for this is considered to have a complicated configuration due to the difficulty of subtracting a light with given intensity from a light with some intensity. Therefore, the present invention further includes a circuit for converting the intensity into delay and performs processes by an optical phase. Then, in the following exemplary embodiments of the present invention, optical intensity is divided into multiple bits from the light as is to obtain a digital value.

Hereinafter, specific exemplary embodiments incorporating the present invention are explained in detail with reference to the drawings. However, the present invention is not necessarily limited to the following exemplary embodiments. Moreover, the following description and drawings are simplified as appropriate for clarity of the explanation.

First Exemplary Embodiment

FIG. 1 is a block diagram of an optical A/D converter according to a first exemplary embodiment. FIG. 1 shows a configuration example of a four-bit optical A/D converter. This optical A/D converter includes an input port 1, an optical splitter 2, optical waveguides 3, Mach-Zehnder (MZ) interferometers 4, output ports 13 to 20, and balanced receivers 9.

The analog input signal Ain, which is an optical signal, is input from the input port 1 and is split by the optical splitter 2 into four equivalent analog signals A3, A2, A1, and A0. This number of split corresponds to the number of bits of the optical A/D converter. Each of the lights split by the optical splitter 2 is input to the MZ interferometer 4 through the optical waveguide 3.

As shown in FIG. 1, the MZ interferometers 4 include four paths that each has one optical splitter 10 and optical coupler/splitter 11. Further, the optical modulation regions 5, 6, 7, and 8 are provided between the optical splitter 10 and the optical coupler/splitter 11 in the respective paths. The four pairs of analog signals A3, A2, A1, and A0 that are split into two arms by the optical splitter 10 are respectively input to the optical modulation regions 5, 6, 7 and 8.

The optical modulation regions 5, 6, 7, and 8 each have two upper and lower inputs and two upper and lower outputs, in which the upper input port is connected to the upper output port and the lower input port is connected to the lower output port. In these regions, the phase of the light passing through the lower input and output ports changes according to the intensity of the optical signal input from the input port 1 as compared to the light passing through the upper input and output ports. Each of the optical modulation regions 5, 6, 7, and 8 is designed to include the amount of phase shift (phase rotation) necessary for outputting a signal corresponding to each bit of the digital signal. Note that the details are described later.

Next, the top path in FIG. 1 is explained as an example, a pair of lights output from the upper and lower output ports through the optical modulation region 5 interferes in the optical coupler/splitter 11. Then, the output light is distributed to the pair of output ports 13 and 14. Similarly, a pair of lights output from the upper and lower output ports through the optical modulation region 6 interferes in the optical coupler/splitter 11, and then distributed to the pair of output ports 15 and 16. A pair of lights output from the upper and lower output ports through the optical modulation region 7 interferes in the optical coupler/splitter 11, and then distributed to the pair of output ports 17 and 18. A pair of light output from the upper and lower output ports through the optical modulation region 8 interferes in the optical coupler/splitter 11, and then distributed to the pair of output ports 19 and 20. Note that although FIG. 1 illustrates that the optical splitter 10 has one input and two outputs, and the optical coupler/splitter 11 has two inputs and two outputs, it is not limited to this.

Next, a pair of lights output from each path of the MZ interferometer is O/E (optical/electrical) converted by the balanced receiver 9. The balanced receiver 9 here is composed of a pair of PDs that are connected in series. Assigning 0 and 1 of a digital signal according to an output from each balanced receiver 9 generates a digital output signal Dout.

Next, an operating principle is explained using FIGS. 2A to 2D. FIG. 2A to 2D are diagrams respectively showing details of the optical modulation regions 5 to 8 in FIG. 1. One arms (upper arms in FIGS. 2A to 2D) in the optical modulation regions 5 to 8 are normal optical waveguides. Light intensity phase conversion units 25, 26, 27, and 28 are respectively provided to the other arms (lower arms in FIGS. 2A to 2D). All of the optical intensity-to-phase conversion units 25, 26, 27, and 28 have linear characteristics as shown in FIG. 3, in which the input optical intensity and the amount of phase shift are in a proportional relationship.

Specifically, the “Kerr effect”, the “self phase modulation effect of a Semiconductor Optical Amplifier (SOA)”, and the like can also be used. When the nonlinear effect is used, the current value of SOA and further, the intensity of the signal light itself should be adjusted in advance to be appropriate to use a linear region as much as possible.

For the sake of simplicity, the optical intensity-to-phase conversion units 25, 26, 27, and 28 shall have the same characteristics per unit length. Additionally, the length of the optical intensity-to-phase conversion unit 25 is determined so that the phase rotation of the optical intensity-to-phase conversion unit 25 will be 2π at certain specified maximum and minimum optical intensity. The length thereof shall be L.

Then, the light transmitting through the MZ interferometer 4 changes in a manner such that delay between the arms of the light modulation region 5 changes from 0 to 2π according to the optical intensity from the minimum optical intensity to the maximum optical intensity. Accordingly, the ratio of output optical intensity B1 from the output port 13 to a total (B1+B2) of the output optical intensity B1 from the output port 13 and output optical intensity B2 from the output port 14 passed through the MZ interferometer 4, which is relative optical intensity B1/(B1+B2), changes as shown in FIG. 4. The horizontal axis in FIG. 4 indicates the input optical intensity and vertical axis indicates the relative optical intensity. FIG. 4 here shows the relative optical intensity on a cross-section 21 in FIG. 1.

Next, the intensity of the output optical intensity B1 and B2 is compared and an evaluation of 0 or 1 should be performed according to which one is greater. Specifically, as the balanced receiver 9 can detect the difference in the output by combining the two PDs, a digital value can be obtained using a comparator. In this way, the digital value like the digital signal D3 in FIG. 5 is obtained according to the input optical intensity.

This ratio is set so that the phase rotation will be 2π according to the optical intensity from the minimum optical intensity to the maximum optical intensity in the optical modulation region 5. Therefore, the repetition period P_(period)=1/f (f is a repetition frequency) will be one period according to the optical intensity from the minimum optical intensity to the maximum optical intensity.

Next, the optical intensity-to-phase conversion units 26, 27, and 28 can be respectively configured to 2L, 4L, and 8L based on the length L of 25, and then the phase rotation of the optical modulation regions 6, 7, and 8 will be 4π, 8π, and 16π according to the optical intensity up to the maximum optical intensity. Accordingly, when the repetition frequency in the above optical modulation region 5 is f, the repetition frequency of the ratio of the output optical intensity from the output port 15 to the total output optical intensity from the output ports 15 and 16 will be 2×f. Similarly, the repetition frequency of the ratio of the output optical intensity from the output port 17 to the total output optical intensity from the output port 17 and output port 18 will be 4×f. The repetition frequency of the ratio of the output optical intensity from the output port 19 to the total output optical intensity from the output port 19 and output port 20 will be 8×f.

In general, to create an n-bit optical A/D converter, the lengths of the optical intensity-to-phase conversion units are set to be longer at less significant bits. Specifically, when the length at the most significant bit is L, the length at each less significant bit shall be 2̂k(k=0, . . . , n-1) times of the length L in order.

Each of outputs from the optical modulation regions 5 to 8 is input to the balanced receivers 9, and digital signals D3, D2, D1, and D0 corresponding to the analog signals A3, A2, A1 and A0 are output. Specifically, the digital signals D3, D2, D1, and D0 as shown in FIG. 5 can be obtained according to the input optical intensity. In other words, the optical intensity of the analog input signal is converted into the digital signal. Note that when the average optical intensity input from the input port 1 is small, the light should be amplified in advance so that the average optical intensity will be close to just the middle value of the digital signal. Moreover, it is desirable to adjust the operating state of the optical intensity-to-phase conversion units 25, 26, 27, and 28 in advance so that the optical intensity is close to the maximum value of the digital signal at the maximum optical intensity and close to the minimum value of the digital signal at the minimum optical intensity.

Second Exemplary Embodiment

Next, a second exemplary embodiment is explained with reference to FIG. 6. FIG. 6 is a configuration example of a four-bit optical A/D converter. The same components as those in FIG. 1 are denoted by the same reference numerals, and the explanation is omitted as appropriate. A local light is not introduced in the optical modulation regions 5, 6, 7, and 8 in FIG. 1 in the first exemplary embodiment. On the other hand, this exemplary embodiment is different in the point that a local light LL3, LL2, LL1, and LL0 is introduced in optical modulation regions 35, 36, 37, and 38.

An analog input signal Ain is input from the input port 1 and split into four equivalent analog signals A3, A2, A1, and A0 by the optical splitter 2. This number of split corresponds to the number of bits of the optical A/D converter. Each light split by the optical splitter 2 is input to the respective optical modulation regions 35, 36, 37, and 38 inside the MZ interferometer 4. Moreover, the local light LL3, LL2, LL1, and LL0 split by the optical splitter 10 into two arms is input respectively to the optical modulation regions 35, 36, 37, and 38.

The optical modulation regions 35, 36, 37, and 38 here each have two upper and lower inputs and two upper and lower outputs, in which the upper input port is connected to the upper output port and the lower input port is connected to the lower output port. In these regions, the phase of the light passing through the lower input and output ports changes according to the intensity of the light signal input from the input port 1 as compared to the light passing through the upper input and output ports. Each of the optical modulation regions 35, 36, 37, and 38 is designed to include the amount of phase shift necessary for outputting a signal corresponding to each bit of the digital signal. Note that the details are described later.

Next, four pairs of lights output from the upper and lower output ports through the optical modulation regions 35, 36, 37, and 38 interfere in the optical coupler/splitter 11. Then, the output light is distributed to the pair of output ports (for example, the output ports 13 and 14). Note that although FIG. 6 illustrates that the optical splitter 10 has one input and two inputs, and the optical coupler/splitter 11 has two inputs and two outputs, it is not limited to this.

In a similar manner as the first exemplary embodiment, the pair of lights output from each path of the MZ interferometer 4 is O/E converted by the balanced receiver 9. The balanced receiver 9 here is composed of a pair of PDs that are connected in series. Assigning 0 and 1 of a digital signal according to an output from each balanced receiver 9 generates a digital output signal Dout.

Next, an operating principle is explained using FIGS. 7A to 7D. FIGS. 7A to 7D are diagrams respectively showing details of the optical modulation regions 35 to 38 in FIG. 6. Optical intensity-to-phase converters 39 are provided in the optical modulation regions 35 to 38. These regions have a function to convert an optical intensity change into delay. The number of these optical intensity-to-phase converters 39 differs for each of the optical modulation regions 35 to 38. Specifically, there is one in the optical modulation region 35, two in the optical modulation region 36, four in the optical modulation region 37, and eight in the optical modulation region 38. In general, to create an n-bit optical A/D converter, the number of the optical intensity-to-phase converters 39 may be 2̂k(k=0, . . . , n-1) in order from more significant bits to less significant bits.

In addition to the local lights LL3 to LL0, analog signals A3 to A0, which are signal lights, are input to the optical intensity-to-phase converters 39 of the optical modulation regions 35 to 38. The phase of the local light is modulated according to the intensity of the signal light to be output.

FIG. 7E is an example of the specific configuration of the optical intensity-to-phase converter 39. A local light LLb (wavelength λ2) input from an input waveguide 44 a of the optical intensity-to-phase converter 39 undergoes a change in the phase according to the intensity of a signal light A (wavelength λ1) input from an input waveguide 44 b in a region 40. Moreover, it is designed in a way that the local light LLb and the signal light A are output separately from the exit of the region 40. Then, the local light LLb is output from an output waveguide 48 through an optical intensity adjuster 42 b. Further, the signal light A is output from an output waveguide 47 through an optical intensity adjuster 41. Additionally, the region 40 is configured so that the phase rotation will be 2π it according to the optical intensity from the minimum optical intensity to the maximum optical intensity.

Specifically, for example, the region 40 has 2×2 MMI (Multi Mode Interference) waveguides that are composed of semiconductor optical waveguides. The width and length thereof are designed so that the light input to the input waveguide 44 a, which is the upper port of the MMI waveguide, is output to the lower output waveguide 48, and the light input to the input waveguide 44 b, which is the lower port, is output to the upper output waveguide 47. Moreover, the semiconductor optical waveguide of this region 40 has a pin structure with electrodes disposed on top and bottom so that current or voltage can be applied thereon. The amount of phase rotation is set to be desirable according to the intensity change of the signal light by this current value and the like.

A local light LLa (wavelength λ2) input to the input waveguide 45 is output from an output waveguide 46 through an optical intensity adjuster 42 a and an optical phase adjuster 43. The optical intensity adjusters 42 a and 42 b and the optical phase adjuster 43 are adjusted so that the relation between the intensity and the phase of the local light input to the input waveguide 45 and the input waveguide 44 a is the same. For example, the optical intensity adjusters 42 a and 42 b are adjusted in advance so that the intensity of the output waveguide 46 and the output waveguide 48 will be the same when the signal optical intensity is the minimum optical intensity. Further, the optical phase adjuster 43 is adjusted in advance so that the phases of the output waveguide 46 and the output waveguide 48 will be the same when the signal optical intensity is the minimum optical intensity. Furthermore, when the optical intensity-to-phase converters 39 are successively connected in cascade as in the optical modulation regions 36, 37, and 38, the optical intensity adjuster 41 is adjusted in advance so that the relation between the signal light and the local light will be the same. In summary, the optical intensity adjuster 41 in the optical intensity-to-phase converter 39 is not necessary in the optical modulation region 35 shown in FIG. 7A. Note that it is preferable that the wavelength λ2 of the local lights LLa and LLb and the wavelength λ1 of the signal light A are different.

Specifically, the optical intensity adjusters 41, 42 a, and 42 b are configured to use SOA and be capable of adjusting a current value thereof as desirable. Moreover, the optical phase adjuster 43 is adjusted to cause desired phase rotation by applying an electric field on the semiconductor light waveguide having the pin structure. In general, the optical intensity adjustment using SOA requires a separate phase rotation adjustor as it involves phase rotation.

With such a configuration, a change in the optical intensity from the minimum optical intensity to the maximum optical intensity causes the phase rotation of 2π in the light modulation region 35, 4π in the light modulation region 36, 8π in the light modulation region 37, and 16π in the light modulation region 38.

Note that in the optical intensity-to-phase converter 39 shown in FIG. 7E, the output positions of the local light and the signal light are reversed in an output part of the region 40. However, it is possible to change the length of the region 40 according to the extent of cross phase modulation of the signal light and the local light and not to reverse the output positions of the local light and the signal light. Such a configuration is shown in FIG. 7F.

Then, similar characteristics as the first exemplary embodiment can be obtained. Specifically, the light transmitting through the MZ interferometer 4 changes in a manner such that delay between the arms of the light modulation region 35 changes from 0 to 2π according to the optical intensity from the minimum optical intensity to the maximum optical intensity. Accordingly, the ratio of output optical intensity B1 from the output port 13 to a total (B1+B2) of the output optical intensity B1 from the output port 13 and the output optical intensity B2 from the output port 14 passed through the MZ interferometer 4, which is relative optical intensity B1/(B1+B2), changes as shown in FIG. 4. Therefore, FIG. 4 shows a ratio calculated based on the optical intensity of the part 21 shown in FIG. 1.

Then, the intensity of B1 and B2 is compared and an evaluation of 0 or 1 should be performed according to which one is greater. Specifically, as the balanced receiver 9 can detect the difference in the output by combining the two PDs, a digital value can be obtained using a comparator.

This ratio is set so that the phase rotation will be 2π according to the optical intensity from the minimum optical intensity to the maximum optical intensity in the light modulation region 35. Therefore, the repetition period P_(period)=1/f (f is a repetition frequency) will be one period according to the optical intensity from the minimum optical intensity to the maximum optical intensity.

Similarly, the light modulation region 36, light modulation region 37, and light modulation region 38 are configured so that the phase rotation will be 4π, 8π, and 16π according to the optical intensity up to the maximum optical intensity. Accordingly, when the repetition frequency in the above optical modulation region 5 is f, the repetition frequency of the ratio of the output optical intensity from the output port 15 to the total output optical intensity from the output ports 15 and 16 will be 2×f. Similarly, the repetition frequency of the ratio of the output optical intensity from the output port 17 to the total output optical intensity from the output port 17 and the output port 18 will be 4×f. The repetition frequency of the ratio of the output optical intensity from the output port 19 to the total output optical intensity from the output port 19 and the output port 20 will be 8×f.

Each of outputs from the optical modulation regions 35 to 38 is input to the balanced receivers 9, and digital signals D3, D2, D1, and D0 corresponding to the analog signals A3, A2, A1 and A0 are output. Specifically, the digital signals D3, D2, D1, and D0 as shown in FIG. 5 are obtained according to the input optical intensity. In other words, the optical intensity of the analog input signal is converted into the digital signal.

Third Exemplary Embodiment

Next, a third exemplary embodiment is explained with reference to FIG. 8. FIG. 8 shows a configuration example of a four-bit optical A/D converter. The same components as those in FIG. 1 are denoted by the same reference numerals, and the explanation is omitted as appropriate. A local light is not introduced in the optical modulation regions 5, 6, 7, and 8 in FIG. 1 in the first exemplary embodiment. On the other hand, this exemplary embodiment is different in the point that a local light LL3, LL2, LL1, and LL0 is introduced in optical modulation regions 55, 56, 57, and 58. This enables improvement in the efficiency of changing the phase according to the light signal intensity.

The function of the optical modulation regions 55, 56, 57, and 58 is similar to that of the optical modulation regions 5, 6, 7, and 8 in FIG. 1, and the optical modulation regions 35, 36, 37, and 38 in FIG. 6. As shown in FIGS. 9A to 9D, the optical modulation regions 55, 56, 57, and 58 respectively include 2̂0=1, 2̂1=2, and 2̂2=4, and 2̂3=8 number of optical intensity-to-phase converters 59. Such a configuration is similar to the one in the second exemplary embodiment and the method of determining the number of inclusion is also similar.

FIG. 9E is an example of a specific configuration of the optical intensity-to-phase converter 59. Regions 60 a and 60 b here include, for example, 2×2 MMI waveguides that are composed of semiconductor optical waveguides. The width and length thereof are designed so that a light input to an upper port of the MMI waveguide is output to a lower part, and a light input to a lower port is output to an upper part. The regions 60 a and 60 b of the same MMI waveguide are respectively provided to both of a lower input waveguide 64 a and an upper input waveguide 65 in the optical intensity-to-phase converter 59. A local light LL (wavelength λ2) is introduced only to the region 60 b of the lower input waveguide 64 a. This enables generation of states with different optical intensity inside the MMI waveguide under the same signal light change. Accordingly, delay can be given to a signal light Aa (wavelength λ1) and Ab (wavelength λ1) that is input to the upper and lower ports using the difference between the self phase modulation and cross phase modulation caused in the MMI waveguide.

Note that also in the optical intensity-to-phase converter 59 shown in FIG. 9E, it is possible not to reverse the output positions of the signal light and the local light in a similar manner as FIG. 7F.

The signal light Aa here input to the input waveguide 65 of the optical intensity-to-phase converter 59 is output from an output waveguide 66 through the region 60 a, an optical intensity adjuster 62, and an optical phase adjuster 63. On the other hand, the signal light Ab input from the input waveguide 64a undergoes a change in the phase according to the intensity of the local light LL input from the input waveguide 64 b in the region 60 b. Moreover, it is designed in a way that the local light LL and the signal light Ab is output separately from an exit of the region 60 b. Then, the signal light Ab is output from an output waveguide 68. Further, the local light LL is output from an output waveguide 67 through an optical intensity adjuster 61.

In a similar manner as the region 40 in the second exemplary embodiment, the semiconductor optical waveguides of these regions 60 a and 60 b have the pin structure with electrodes disposed on top and bottom so that current or voltage can be applied thereon. As described so far, disposing the optical intensity-to-phase converter 59 in the manner shown in FIGS. 9A to 9D obtains the digital signals as in FIG. 5.

Note that in the first to third exemplary embodiments, the length of the optical intensity-to-phase conversion units 25 to 28 and the number of the optical intensity-to-phase converters 39 and 59 are set based on the binary code. In practical, different values are set appropriately according to the format of the digital signal code.

For example, the optical modulation regions 5 to 8 in the first exemplary embodiment should have the configurations shown in FIGS. 10A to 10D in order to output Gray codes shown in FIG. 12. The optical phase modulator 50 rotates the phase by π/2 without changing the optical intensity. In this case, to create an n-bit optical A/D converter in general, assuming that the length of the optical intensity-to-phase conversion units of the most significant bit is L, the lengths of the optical intensity-to-phase conversion units to which signals of each bit are output should be 2̂k(k=0, 0, 1, 2, 3, . . . , n-2) times of the length L from more significant bits to less significant bits. The length of the optical intensity-to-phase conversion unit can be shorter than in the case of binary code.

Specifically, the optical phase modulator 50 here should cause desired phase rotation by applying an electric field on the semiconductor optical waveguide having the pin structure. Further, it is possible to achieve to change the waveguide length by π/2 as the optical path length. Such a configuration obtains digital outputs as shown in FIG. 12 according to the input optical intensity.

In the second exemplary embodiment, the optical modulation regions 35 to 38 may be configured as in FIGS. 11A to 11D to enable output of the Gray codes shown in FIG. 12. The optical phase modulator 50 here rotates the phase by π/2 without changing the optical intensity. In general, to create an n-bit optical A/D converter, the number of the optical intensity-to-phase converters 39 may be 2̂k(k=0, 0, 1, 2, 3, . . . , n-2) in order from more significant bits to less significant bits. The number of the optical intensity-to-phase converters 39 can be made less than the case of binary code. In a similar manner, in the third exemplary embodiment, the optical modulation regions 55 to 58 may be configured as in FIGS. 11A to 11D to enable output. This optical phase modulator 50 can also be realized by a similar method as the optical phase modulator 50 in the above FIGS. 10A to 10D.

Note that it is needless to say that the above exemplary embodiments can be combined within the range not contradicting the contents thereof. Although the abovementioned exemplary embodiments and modifications explained the configuration of each part in detail, the configuration can be modified in the range satisfying the present invention. According to the present invention, as the high speed and low power optical A/D converter can be realized, it is possible to use the optical A/D converter in the optical modulation circuit taking advantage of high speed and low power. Specifically, the optical A/D converter of the present invention can be included in a coherent detection circuit and an optical direct detection circuit.

Although the present invention has been explained with reference to the exemplary embodiments, the present invention is not limited by above. Various modifications that can be understood by a person skilled in the art can be made to the configurations and details of the present invention within the scope of the invention.

The present application claims priority rights of and is based on Japanese Patent Application No. 2010-115544 filed on May 19, 2010 in the Japanese Patent Office, the entire contents of which are hereby incorporated by reference.

INDUSTRIAL APPLICABILITY

The technique according to the present invention can be used for an optical analog-to-digital converter, an optical signal demodulator and an optical modulator-demodulator using thereof, the optical analog-to-digital converter and the like that are used in an optical communication system or optical interconnection.

REFERENCE SIGNS LIST

-   1 INPUT PORT -   2 and 10 OPTICAL SPLITTER -   3 OPTICAL WAVEGUIDE -   4 MZ INTERFEROMETER -   5 to 8, 35 to 38, 55 to 58 OPTICAL MODULATION REGION -   9 BALANCED RECEIVER -   11 OPTICAL COUPLER/SPLITTER -   13 to 20 OUTPUT PORT -   21 CROSS-SECTION -   25 to 28 OPTICAL INTENSITY-TO-PHASE CONVERSION UNIT -   39 and 59 OPTICAL INTENSITY-TO-PHASE CONVERTER -   40, 60 a, and 60 b REGION -   41, 42 a, 42 b, 61, and 62 OPTICAL INTENSITY ADJUSTOR -   43 and 63 OPTICAL PHASE ADJUSTER -   44 a, 44 b, 45, 64 a, 64 b, and 65 INPUT WAVEGUIDE -   46 to 48 and 66 to 68 OUTPUT WAVEGUIDE -   50 OPTICAL PHASE MODULATOR 

1. An optical A/D converter comprising: an optical splitter that splits an input analog optical signal into a plurality of optical signals; a plurality of Mach-Zehnder interferometers, each of the plurality of optical signals split by the optical splitter being input to the plurality of Mach-Zehnder interferometers; plurality of optical/electrical conversion unit that convert each optical signal output from each Mach-Zehnder interferometer into a digital electrical signal, wherein each Mach-Zehnder interferometer comprises optical intensity-to-phase conversion unit that optically converts intensity of the input optical signal into an amount of phase shift, and the amount of phase shift differs for each Mach-Zehnder interferometer.
 2. The optical A/D converter according to claim 1, wherein the optical intensity-to-phase conversion unit is a semiconductor optical amplifier.
 3. The optical A/D converter according to claim 1, wherein each Mach-Zehnder interferometer comprises: an internal optical splitter that splits an input light into two; first and second waveguides that are connected to the internal optical splitter; and a coupler/splitter that is connected to the first and second waveguides, and the optical intensity-to-phase conversion unit is provided to at least the second waveguide and delay from the first waveguide can be given.
 4. The optical A/D converter according to claim 1, wherein the amount of phase shift differs because of a length of each optical intensity-to-phase conversion unit that is different for each Mach-Zehnder interferometer.
 5. The optical A/D converter according to claim 1, wherein the amount of phase shift differs because of the number of the optical intensity-to-phase conversion unit that is different for each Mach-Zehnder interferometer.
 6. The optical A/D converter according to claim 1, wherein the optical intensity-to-phase conversion unit is composed of a balanced receiver including two photodiodes connected in series.
 7. The optical A/D converter according to claim 1, wherein the Mach-Zehnder interferometer further comprises a local light introduction waveguide being input with a local light having a wavelength different from a signal light.
 8. An optical signal demodulator comprising the optical A/D converter according to claim
 1. 9. An optical modulator-demodulator comprising the optical signal demodulator according to claim
 8. 10. A method of constructing an optical A/D converter comprising: providing an optical splitter that splits an input analog optical signal into a plurality of optical signals; providing a plurality of Mach-Zehnder interferometers, each of the plurality of optical signals split by the optical splitter being input to the plurality of Mach-Zehnder interferometers; providing plurality of optical/electrical conversion unit that convert each optical signal output from each Mach-Zehnder interferometer into a digital electrical signal; providing optical intensity-to-phase conversion unit to each Mach-Zehnder interferometer, the optical intensity-to-phase conversion unit optically converting intensity of the input optical signal into an amount of phase shift; and performing construction so that the amount of phase shift will be different for each Mach-Zehnder interferometer.
 11. An optical A/D converter comprising: an optical splitter that splits an input analog optical signal into a plurality of optical signals; a plurality of Mach-Zehnder interferometers, each of the plurality of optical signals split by the optical splitter being input to the plurality of Mach-Zehnder interferometers; plurality of optical/electrical conversion means that convert each optical signal output from each Mach-Zehnder interferometer into a digital electrical signal, wherein each Mach-Zehnder interferometer comprises optical intensity-to-phase conversion means that optically converts intensity of the input optical signal into an amount of phase shift, and the amount of phase shift differs for each Mach-Zehnder interferometer. 